363697 The parameter used to measure the stability of the nucleus is

363698 Consider the nuclear reaction:
\(X^{200} \rightarrow A^{110}+B^{90}+\) Energy
The binding energy per nucleon for \({X^{200}},{A^{100}},{B^{90}}\) are respectively \(7.4\,MeV,8.2\,MeV\) and \(8.2\,MeV\). The energy released is

363699 Assertion :
If a heavy nucleus is split into two medium sized parts, each of the nuclei will have more binding energy per nucleon than the original nucleis.
Reason :
Joining two light nuclei together to gives a single nucleus of medium size means more binding energy per nucleon than the two nuclei.

363700 Following process is known as \(h \nu \longrightarrow e^{+}+e^{-} \quad\)

363697 The parameter used to measure the stability of the nucleus is

363698 Consider the nuclear reaction:
\(X^{200} \rightarrow A^{110}+B^{90}+\) Energy
The binding energy per nucleon for \({X^{200}},{A^{100}},{B^{90}}\) are respectively \(7.4\,MeV,8.2\,MeV\) and \(8.2\,MeV\). The energy released is

363699 Assertion :
If a heavy nucleus is split into two medium sized parts, each of the nuclei will have more binding energy per nucleon than the original nucleis.
Reason :
Joining two light nuclei together to gives a single nucleus of medium size means more binding energy per nucleon than the two nuclei.

363700 Following process is known as \(h \nu \longrightarrow e^{+}+e^{-} \quad\)

363697 The parameter used to measure the stability of the nucleus is

363698 Consider the nuclear reaction:
\(X^{200} \rightarrow A^{110}+B^{90}+\) Energy
The binding energy per nucleon for \({X^{200}},{A^{100}},{B^{90}}\) are respectively \(7.4\,MeV,8.2\,MeV\) and \(8.2\,MeV\). The energy released is

363699 Assertion :
If a heavy nucleus is split into two medium sized parts, each of the nuclei will have more binding energy per nucleon than the original nucleis.
Reason :
Joining two light nuclei together to gives a single nucleus of medium size means more binding energy per nucleon than the two nuclei.

363700 Following process is known as \(h \nu \longrightarrow e^{+}+e^{-} \quad\)

363697 The parameter used to measure the stability of the nucleus is

363698 Consider the nuclear reaction:
\(X^{200} \rightarrow A^{110}+B^{90}+\) Energy
The binding energy per nucleon for \({X^{200}},{A^{100}},{B^{90}}\) are respectively \(7.4\,MeV,8.2\,MeV\) and \(8.2\,MeV\). The energy released is

363699 Assertion :
If a heavy nucleus is split into two medium sized parts, each of the nuclei will have more binding energy per nucleon than the original nucleis.
Reason :
Joining two light nuclei together to gives a single nucleus of medium size means more binding energy per nucleon than the two nuclei.

363700 Following process is known as \(h \nu \longrightarrow e^{+}+e^{-} \quad\)